[0001] The present invention concerns a method for controlling the power delivery to a pair
of induction heaters/coils belonging to a household cooking hob. Induction cooking
appliances rely on the inductive effect to heat cooking vessels placed on their cooking
surfaces. Vessel heating occurs by the inductive coupling of the metallic pan with
the time-varying magnetic field generated by the appliance.
[0002] The basic functional architecture implemented into an appliance for generating the
electromagnetic field comprises at least one inductor for each cooking zone of the
induction heaters (including a metallic coil commonly referred as "pancake"), an electrical
power generator to supply the coils, an electronic control unit to supervise the power
delivered by the coils, and and to execute the user settings inputted through the
user interface.
[0003] The so-called "eddy currents" are induced in the bottom side of the metallic pan
from the electromagnetic field generated by the inductor coil. The electronic control
unit supervises the power delivered to the coil by means of a high frequency driving
signal. The driving signal controls the operations of an electronic AC-AC converter
(hereafter referred to as "converter") provided with solid-state switches (Insulated
Gate Bipolar Transistor-IGBT, or the like) that supplies the coils with a suitable
AC current. Consequently, the coil generates, in the surrounding space, a time-varying
electromagnetic field whose amplitude and frequency determine the amount of power
delivered to the pan. The induced currents find in the vessel bottom an electrical
resistance R which depends mainly from the material characteristics and from the electromagnetic
field penetration depth (namely, skin effect). The induced currents generate heat
according to the Joule effect.
[0004] Several circuits are known to generate such time-varying electromagnetic field but,
as consequence of the typical operating frequencies and considering the power normally
delivered by a single heater (ranging from 0 to 3 kW), two main resonant converter
circuits are commonly adopted: the resonant Half-Bridge (HB) converter (Fig.2), and
the Quasi-Resonant (QR) converter (Fig.3). The driving signals of these converters
typically ranges from 20 kHz to 50 kHz.
[0005] These converters, thanks to solid state switches like IGBT, convert the static rectified
DC-link voltage into a squared voltage waveform that supplies a resonant RLC circuit,
wherein L is the impedance of the coil, C is the resonant capacitor and
[0006] R is the circuit resistance, linked with the pan characteristics.
[0007] In the case of the HB topology, the resonant "tank" circuit (the L and C of the resonant
circuit) is defined by the inductor coil L1 and the two resonant capacitors C1 and
C2. A driving signal S1 shaped as square waveform with frequency f
HB switches, directly or through a switching logic SL, two IGBT's (SW1 and SW2), alternating,
within the control period T, the voltage applied to the resonating circuit. The signal
O
1 of the HB converter during the control period T, is a forcing oscillator. The alternate
current flowing through the coil L1 induces the time-varying electromagnetic field
in the surrounding area, necessary for heating the above placed pan.
[0008] In the case of the QR topology, L2 and C3 define the resonant "tank" circuit. The
single IGBT (SW4) of the circuit is driven with a squared wave signal (S2) generated
by the electronic control, energizing the circuit output (O
2) during the T
ON portion of the driving period T only, and leaving the circuit output (O
2) free to oscillate during T
OFF. In fact, during T
ON the IGBT conducts and the coil L2 is charged from the static DC-link voltage while,
in the following time of the period T when IGBT is open, the circuit is freely oscillating
as a damped harmonic oscillator. T
OFF is therefore defined as the time elapsed between the end of T
ON and the time instant when the oscillating current flowing trough the capacitor C3,
or the voltage across its terminals, crosses the zero value for the first time. T
OFF is therefore linked by the physics of the oscillator with the selected T
ON, the free oscillation being determined by the system L2, C3, R (when the pan is superposed
to the coil) in which the initial oscillating conditions are defined by the charge
of the coil L2 (load) accumulated during T
ON. The power supplied by the pancake coil L2 is therefore set by choosing the proper
T
ON time.
[0009] In other equivalent embodiments T
OFF can be intended as the time elapsed between T
ON and the time instant for which the voltage across the coil L2 crosses the zero value
for the first time.
[0010] It is here pointed out that the output signals of the AC converters are not normally
regular sinusoids. For this reason, in the following description when an AC frequency
is mentioned, is intended to refer to the signal fundamental frequency, in the meaning
of signal spectral analysis.
[0011] The fundamental operating frequency of the AC signal outputted by the converter is
therefore given by f
QR = 1/(T
ON + T
OFF).
[0012] For a HB converter, the power transfer characteristic of the coupled systems, that
is the relationship between the power P delivered from the heater to a superposed
cooking utensils, pots, pans, casseroles or the like and the frequency f
HB of the driving signal generated by the electronic control unit, resembles the shape
typical of lightly damped forced harmonic oscillator.
[0013] For a QR converter, the output power P is in a direct relationship with the switching
frequency f
QR, once T
ON is established, and the related power transfer characteristic of the coupled systems
represents this link. Also in this case, the power transfer characteristic of the
coupled systems resembles the typical shape of lightly damped forced harmonic oscillator.
[0014] For both the converter topologies the damping oscillator factor is provided with
the resistance R, specific of each pan, "mirrored" into the pancake through the inductive
coupling.
[0015] For avoiding the IGBT damages and to increase the converter efficiency (that means
reducing the power dissipated during the switching operations), in both the converter
topologies the IGBT's must be switched in the narrow time window when the voltage
across the IGBTs is crossing the zero. Sometime the IGBTs are also protected against
over currents by applying snubbing networks in parallel.
[0016] The main advantage of the QR topology compared with the HB topology is in its lower
cost, due to the reduced number of components. Disadvantages are in the tight time
switching to which the IGBT is subjected.
[0017] A problem affecting both the topologies when operating in pairs in order to activate
simultaneously two induction heaters, in a not coordinated and optimized way, is the
occurrence of a too frequent light flickering and, more generally, a non compliance
with the regulations concerning the requirements for the electromagnetic induced emissions.
[0018] Another problem affecting both converter topologies is the onset of beat noise that
may occur when two or more converters are connected to the same power line filter
when driving signal operate at different frequencies. In particular, when two induction
heaters/coils are activated for heating at the same time two vessels placed on the
hob, their converters need to be driven at proper frequencies in order to deliver
to the vessels the requested power. Whenever these frequencies differ from less than
the maximum audible frequency (around 16kHz), the shared line filter may produce mechanical
vibration. An audible whistling noise may therefore annoy the user.
[0019] Some of the problems above mentioned have been addressed and solved by implementing
specific solutions. Two of these solutions are hereafter summarized.
[0020] In
WO 05/043737A2 it is described an asymmetrical duty cycle control method for driving two HB converters
connected to respective induction coils, operating at the same time, for delivering
to each of the two superposed vessels a preset amount of power.
[0021] The control method disclosed consists in keeping constant the frequency of the squared
waveform driving signal (S1 in Fig. 2) for each of the two HB converters and adjusting
in a proper way, the duty cycle of the two IGBT gate signals (S1
A for Gate_A1, S1
B for Gate _A2 in fig.2), allowing each coil (induction heater) to deliver the preset
amount of power to its superposed vessel. It is known when a duty cycle is changed
from its value of 50%, to a lower or higher value, the r.m.s. voltage applied to the
coil is reduced, leading to an output power lower than that obtainable at 50%value
of duty cycle (which is the Pmax value deliverable to the superposed vessel by this
system).
[0022] The regulation ratio, which is the ratio Pmax/Pmin, wherein Pmin is the minimum power
deliverable to the vessel by the system using the duty cycle modulation, is lower
than 3:1.
[0023] When the difference between the power to be delivered by the two coils is too large
to be accommodated by the duty cycle modulation only, the driving frequencies of the
two coil/burners are displaced of, at least, 17kHz apart.
[0024] The use of an additional control parameter (duty-cycle) in the HB converter topology
makes possible to extend the range of allowed output power levels and prevents the
onset of beat noise when multiple heaters are operated at the same time. On the other
side, the asymmetrical gate driving leads the converter towards a lower efficiency
resulting in heat dissipated during the switching operation, because the snubbing
network required to prevent this phenomena can be tailored only for a given switching
duty cycle. Moreover, the electrical and thermal stresses on the two IGBTs are unevenly
distributed. Finally, the PWM (Pulse Width Modulation) generation with unsymmetrical
duty cycle is not a cost-effective solution.
[0025] From
EP 0286044 it is disclosed an AC-AC single converter circuit, either HB or QR type, shared to
feed two induction heaters/coils, alternatively connected by means of a relay switch.
With this circuit configuration, low power levels can be delivered acting an ON-OFF
modulation when switching between the two coil elements, keeping active at the fixed
power each element for the time required to deliver the net average power required.
The beat noise is inherently avoided by alternatively driving only one of the coils.
Such approach presents several drawbacks.
[0026] The appliance may cause annoying light flicker due to the frequent changes in drained
current from the mains.
[0027] The power according to this method is not delivered in a smooth way modality. In
fact, when the ON-OFF modulation is too slow, the commutation could be perceived from
the user especially at low power levels, because these levels are implemented by outputting
a relatively large amount of power for a short time, which could potentially damage
the cooked food. When otherwise both the heaters are operated at high power level,
the user may perceive the switching between the elements, seeing the water boiling
and then stopping.
[0028] Another way to achieve the independent power regulation when using two HB converters
working at the same frequency, is to include upstream each converter a DC-Bus voltage
regulator like a well known step-up (boost), step-down (buck), Buck-Boost or similar.
This approach is commonly used in industrial applications but is nearly absent in
consumer applications because of the increase of cost, power dissipation, and the
space occupied by the additional power conversion stage.
[0029] An object of the present invention is therefore to provide a method that does not
present the drawbacks of the prior art. More specifically, the method according to
the present invention enables the simultaneous operation of two induction heaters
avoiding the occurrence of beat noise while providing a smooth delivery of the preset
power levels. The method is then not limited by the intrinsic characteristics of the
converter and coil assembly, being applicable to the HB and QR converter topologies
and to similar topologies or those derived therefrom. In a further step the method
can be refined by selecting among the possible working modalities, the one that optimizes
one or more additional working parameters as the minimization of the light flickering
effect, the minimization of the component stress, or the overall efficiency.
[0030] The method can be applied using slow and fast time scales and prevents the onset
of flicker noise.
[0031] Other features and advantages of the present invention will become readily apparent
from the following detailed description and example when read in light of the accompanying
drawings, in which:
- figure 1 shows a schematic sectional view of an induction cooking hob;
- figure 2 shows the schematic of a Half Bridge converter topology circuit, known in
the art;
- figure 3 shows the schematic of a Quasi Resonant converter topology circuit, known
in the art;
- figure 4 is a representation of the functional architecture for an induction cooking
hob according to the present invention;
- figure 5 shows the power characteristic curves of two heaters according to the invention;
- figure 6 shows a graphical diagram of the power delivered by two induction heaters
during a control period , when the heaters are driven according to the method of the
present invention;
- figure 6A shows one of the possible embodiments of the method according to the present
invention, in which the activation sequence of the two induction heaters, is shown
during two consecutive control periods;
- figure 7 shows another embodiment of the method wherein the control period comprises
a third time fraction;
- figure 8 is a diagram of a finite number of calculated solutions plotted vs. duty
cycle %;
- figure 9 is another diagram of the same data shown in fig. 8 highlighting the solution
chosen to optimize the light flickering parameter;
- figure 10 shows the diagram of fig.8 wherein the chosen solutions are highlighted;
- figure 11 is a schematic flow chart of a possible implementation of the method according
to the present invention, and
- figure 12 is the representation of a further embodiment of the method according to
the present invention.
[0032] With reference to the drawings, an induction hob 10 is provided with a glass ceramic
surface 20 or the like, an user interface (not shown) two induction heaters/coils
A, B, (also known as burners) and a common control circuit 90 provided with two converters
40, 45 (this architecture is also named as twin converters configuration) for driving
the two heaters/coils A, B in a coordinated way. Each converter 40, 45 can be of the
known type, based either on the HB (shown in Fig.2) or on the QR topology, (shown
in Fig.3) or derived from these types.
[0033] In a different hob configuration (not illustrated) more pairs of induction heaters
are included in the same hob and the control circuit is designed to drive, in a coordinated
way, each pair of coils A, B. In another (not illustrated) hob configuration, two
induction coils A,B driven according to the present method define an induction heater
provided two heating zones.
[0034] Two cooking utensils C1, C2 as like pots, pans, casseroles or the like, are placed
on the hob surface 20 in correspondence to the underneath induction heaters/coils
A, B. The levels of power PA
0 PB
0 to be delivered, respectively, from heater A and
[0035] B to their superposed cooking utensils C1 and C2, are set in the electronic control
unit before to start operating, in direct relationship with the inputs received from
the user through the user interface. The power levels PA
0 PB
0of the two heaters A, B can be set for example at PA
0=2.5kW and PB
0=800W.
[0036] The method of the present invention is a control algorithm allowing two induction
heaters/coils A, B to simultaneously deliver the preset power levels PA
0 PB
0, on average over the control period T, to their respective superposed cooking utensils
C1, C2 by driving their single converters in a coordinated way. The method is substantially
an "open-loop" control, relying on the assumptions that the power characteristic curves
of the two induction heaters A, B are known.
[0037] Generalizing the definition given above, the power characteristic curve is the relationship
between a characteristic of the signal S1, S2, driving the converter 40, 45, which
is an adjustable periodic driving signal S1, S2, and the power PA, PB delivered to
the specific superposed cooking utensil C1, C2 in the operating range of the induction
heater A, B. The characteristic of the periodic driving signal S1, S2 to be considered
in the construction of the characteristic curves depends from the type of converter
40, 45 used and could be, for instance, f
HB in the case of the HB converters 40 or f
QR, with a certain T
ON-T
OFF, for the QR converters 45 types. In an equivalent way, other characteristics of the
driving signals S1, S2 can be used for the construction of the power characteristic
curve.
[0038] A convenient selection of the control period T is then made with the aim to obtain
a smooth heat delivery. In a preferred embodiment the control period T is lower than
the thermal time constant Tau of the superposed cooking utensils (C1, C2), which is
normally not lower than 12 seconds, to provide a smooth power delivery to the superposed
cooking utensils (C1,C2). According to this, a convenient control period can be set,
for instance as T= 5 sec.
[0039] T value can also be chosen to be a multiple of the half period of the power supply
network.
[0040] In the example described in Fig.1 to 4, two equals induction heaters are connected
with two converters. The first heater A is connected to a HB converter 40, while the
second heater B is connected to a QR converter 45. In others embodiments (not described)
both the induction heaters/coils can be connected to converters belonging to the same
topology, either HB, QR or similar and derived. In different embodiments the power
dimension for the two heaters A, B may also be not necessary equal.
[0041] In order to apply the method of the present invention, it is required to build, for
each of the two heaters/coils A, B coupled with their superposed cooking utensil C1,
C2, its specific power characteristic curve. This operation has to be performed when
a cooking utensil is placed the first time on the hob surface, above the induction
heater, prior to its activation.
[0042] In an example of implementation of the method according to the present invention,
for the first heater A the power characteristic curve PA=F
C1(f
HB) is created by first mapping the power delivered by the induction heater to the superposed
cooking utensil C1, over a certain number of frequencies distributed in the frequency
range for which the induction system has been designed to operate.
[0043] This power mapping is achieved by stepping on the frequency f
HB of the signal S1 driving the HB converter in the operating range f
HB1, f
HB2...f
HBN and determining the associated power outputs PA
fHB1, PA
fHB2,. PA
fHBN for each step 1, 2.. N with any of the known methods (i.e. shunt resistors, etc.).
[0044] For the burner B, in a similar manner, the power transfer characteristic related
to the superposed cooking utensil C2 is PB=F
C2(f
QR,T
ON), or in an equivalent way PB=F
C2(T
ON,T
OFF), and is built stepping T
ON of the driving signal S2 over the heater operating range, reading T
OFF with the time counter of the electronic control unit, and determining the corresponding
power outputs PB
fQR1, PB
fQR2, ..PB
fQRN is calculated by the control unit 90.
[0045] After the mapping operation, the whole power characteristic curves PA=F
C1(fHB) and PB=F
C2(f
QR,T
ON) or PB=F
C2(T
ON,T
OFF), related to the specific superposed cooking utensils C1,C2, can be reconstructed,
when required, interpolating the single sampled points using one of the known numerical
methods, for instance the 5
nd order polynomial method. The characteristic curves are then memorized into the memory
of the control unit 90 in the form of lookup tables, or either in equation form.
[0046] The characteristic curves PA=F
C1(f
HB) of the first heater A and PB=F
C2(f
QR), or PB=F
C2(T
ON,T
OFF) for the second heater B, are plotted in Fig. 5.
[0047] It is here pointed out that, to cope with slow variations of the power transfer curve
due to changes of the load impedance (due to pot heating, pot movement etc.), the
system may need to check continuously the consistency of it's stored power transfer
curve with the actually delivered power in order to trigger a new acquisition of such
curve upon the evidence that a substantial calculated deviation DE has occurred since
the last acquisition. In one example of implementation, the amount of deviation DE
that may be tolerated before a new acquisition is deemed to be required is directly
related to the desired accuracy of the power control and may be preferably set in
the range of 2% to 10% or relative error. A threshold error T
HE for comparing the calculated deviation DE can therefore be set, i.e. T
HE= 5% of relative error. When the deviation DE is greater that the threshold error
T
HE, the power characteristic curve P=F
C1(f
HB), P=F
C2(f
QR), or P=F
C2(T
ON,T
OFF) is newly built.
[0048] It is also pointed out that in some embodiments of the present method, standards
power characteristic curves related to standard cooking utensils to be used on the
hob can be stored into the control unit memory of the electronic control 40 during
the manufacturing phase and therefore, when the related cooking utensil is recognized,
one or more among the memorized curves are used.
[0049] In the case when only one single cooking utensil C1 or C2 need to be heated, the
controls 40 activates its induction heater, A or B by applying to the converter 40
45 to which the heater is connected a proper driving signal S1, S2, in order to allow
the induction heater to deliver to the superposed cooking utensil C1 C2, the preset
power level PA
0 or PB
0. The characteristics of this proper signal S1, S2 are calculated form the power characteristic
curve of the single induction heater, previously generated, directly or by interpolating
the mapped points.
[0050] In the example described in fig. 4, 5, 6, 6A, 8, 9, 10, heating the first cooking
vessel C1 superposed to the first heater A without operating the burner B (heater
B switched OFF), requires to drive the HB converter with a driving signal S1 operating
at a frequency of f
HBPA0=24 kHz while, in the same way, heating the second cooking vessel C2 superposed to
the second heater B without operating the burner A, requires to drive the QR converter
with a driving signal S2 operating at the frequency f
QRB0= 26 kHz wherein T
ON= 15 µsec.
[0051] When both the cooking utensils C1 C2 need to be heated at the same time, the method
according to the present invention is applied. According to this method two induction
heaters A, B deliver the preset power PA
0, PB
0, on average over the period T to their respective cooking utensils C1 C2, by driving
the two converters with their respective periodic signals S1, S2 including a two-fractions
sequence, illustrated in Fig.6, 6A, for which:
- during a first fraction T1 of the period T, both the induction heaters A and B are
simultaneously activated driving their converters 41, 44 with a signal S1, S2 operating
at the same first frequency f1, that means fQR=f1 and fHB=f1;
- during a second fraction T2 of the period T, one of the two induction heaters A,B
is turned off halting its driving signal S1, S2, while the other heater continues
to operate driven its converter with a signal S1, S2 operating at a second frequency
f2.
[0052] Of course also the inverted sequence in which T2 precedes T1 is included in the present
invention, since it is not important the order of the time fractions T1, T2 within
the control period T, rather than their occurrence.
[0053] The induction heater which is to be switched off among the two A, B during the second
fraction T2 is the one that, if operating alone (with the other heater switched off)
at the requested power level, would require a driving signal presenting the highest
frequency. According to the typical shape of the power characteristic curves, the
heater to be switched off is normally the one that has to supply the lower power level
among two equal induction heaters.
[0054] In the described example, being the first heater A driven with a signal S1 operating
at f
HBPA0=24 kHz in order to supply a power of 1,5 kW to its superposed cooking utensil C1,
and being the second heater B driven with a signal S2 operating at
[0055] F
QRB0= 26 kHz with T
ON= 15µsec in order to supply a power of 1 kW to its superposed cooking utensil C2,
the heater that will be switched off during the second fraction of the control period
T2 is the second heater B.
[0056] In Fig.5 the frequencies f
HBPA0=23 kHz and F
QRB0= 34 kHz, satisfying the predetermined powers levels PA
0 and PB
0, are represented on the respective power characteristic curves P
C1=F
C1(f
HB), and P=F
C2(f
QR), or P=F
C2(T
ON,T
OFF) related to the induction heaters A, B coupled with their superposed cooking utensils
C1, C2.
[0057] In the preferred embodiment of the method according to the present invention T=T1+T2,
wherein T1 can precede T2 or vice versa. In a different, not described method application,
T1 and T2 are continuously alternated in the consecutive driving periods T during
the heaters time activation, being T1 preceding T2 in the first control period T,
while, in the following control period T, T2 is preceding T1, and so on.
[0058] There could be also a case, in another method embodiment shown on Fig.7 in which
there exists also a third fraction T3 of the period T, located within the same period
T, in which both the induction heaters are switched off. This is the case when it
is requested to regulate the burners at very low power levels for which the frequency
of the driving signals S1, S2 should be too high for switching the solid state switches.
In such case a low (average) power is supplied to the cooking utensils, by reducing
the activation time of the heaters over the period T, introducing a dead time, which
is the third fraction T3. In this case T =T1 +T2 +T3.
[0059] In the preferred embodiment, once defined D =T1/T, the calculation of the first frequency
f1, of the signals S1, S2 driving both the converters of the induction heaters A,
B during the first fraction T1, and the calculation of the second frequency f2, of
the signal S1, S2 driving the single converter of one induction heater during the
second fraction T2 of the period T, come out from the solution of the following set
of equations:

[0060] One preferred way to solve the above set of equations is "to sweep" the parameter
D over a number
n of discrete steps in the range of [0..1]. For each of these steps | a solution of
the above system of equations is then searched. Each solution, when existing, is defined
by a set of three values of the parameters {D=
Dn, f1=
f1n, f2= |
f2n}, each solution fulfilling the power requests of PA
0 and PB
0 over the control period T. A subset of these solutions, evenly distributed in the
admitted operating range, can be calculated with known algebraical methods. This calculation
is easily performable with a processor normally used for commercial appliances, requiring
few instants of CPU time.
[0061] In the example, a calculation of a number of allowed solutions has been performed.
The calculated solutions are plotted in Fig 8, wherein the horizontal axis shows D.
[0062] The calculated solutions can be stored into the memory of the electronic control
unit 90 for further processing. In fact, the choice of one solution among the whole
set of available solutions may be done applying one or more optimization criteria.
[0063] It is here highlighted that choice of driving the two induction heaters/coils A,
B together in the first fraction T1 with driving signals S1, S2 operating at the same
first frequency f1, avoids any occurrence of acoustic noise perceived from the users
during the heating operations. For the second fraction T2 the problem is not present,
having only one heater operating.
[0064] In a further step of the method, additional criteria can be applied with the aim
to select, among the admitted solutions, the one that optimizes one or more working
parameters of the circuit. These parameters depend from the type of installation chosen
for the appliance and related for instance, with the minimization of power losses
across the solid state switches during the switching operation, or with the reduction
of the component's stress, or with the minimization of the light flickering when switching
between the fractions T1, T2 (and eventually with the third fraction T3 of the period
T).
[0065] As consequence, when any of the mentioned optimization criterion is established,
it is defined another functional relationship (in the form of equation or lookup table)
between the characteristics of the driving signal S1, S2 and a functional parameter
linked with the optimization criteria.
[0066] The combination of the new constraints defined by the functional relationships with
the set of equations previously described provides a subset of solutions that optimize
the functional parameter, and consequently the criteria. More than one criterion can
be applied in determining the optimized solutions f1
OPT and f2
OPT.
[0067] In fig. 9 curves are plotted representing some examples among the optimizing criterion.
[0068] The final choice of the first frequency f1= f1
OPT and of the second frequency f2= f2
OPT can be finally done.
[0069] In the example, as highlighted in Fig. 9 and 10, the optimized solution f1
OPT, f2
OPT, D chosen is the one that satisfies, in the most favorable way, the criterion of
the minimum light flickering. Finally, it results that f1= f1
OPT= 25,8kHz, f2= f2
OPT= 21,8kHz, D=43%
[0070] It is then pointed out that normally the value of the calculated first frequency
f1, f1OPT, is different from the value calculated for the second frequency f2, f2OPT
but, in some specific cases, they could be identical.
[0071] Once a suitable solution among the available set has been identified, expressed in
terms of the three outputs: f1, f2, D (being D1= T1/T), wherein D is a real number
ranging from 0 to 1 [0,1], a further refinement of the present invention can be applied.
[0072] In practice, any digital implementations of both ON/OFF and PWM control algorithm,
applies some form of quantization of the time Δt , which is the time quantization
of T or time slice, to the solution D, thus becoming a rational number <D1>. For instance,
assuming the solution for D=0.37, and having chosen T= 5 seconds and choosing Δt =
0.25 seconds, the closest available Duty Cycle <D1> would be equal to 0.35 (0.35=
round (0.37/(0.25/5)).
[0073] If choosing the time slice Δt synchronized with the power supply network and equal
to the half of the duration of the power supply network period, i.e. 10 msec., it
is possible to apply driving signals S1, S2 providing with control patterns as the
one described in the so called "cycle skipping" method. Such method is well known
in the art and described in
US 4871961. This document discloses a method of controlling the supply of power to electrical
loads with a minimum of switching surges, while providing finer power control.
[0074] According to this, the method according to the present invention has to include the
following additional steps, before to be executed (shown in fig. 12):
- find the best approximation of the required Duty Cycle <D1> with the given choice
of Δt/T calculating: <D1>=round(D/(Δt/T), wherein <D1> is the quantized value of D.
- Slice the control period T according to the 10ms quantization.
- Permute the slice order
[0075] In a preferred embodiment, the permutation of the slice order is performed with a
first step consisting in sorting the slices of the control period T according to their
overall power values (applying sorting criteria according either to an increasing
or a decreasing value), wherein the overall power value for each slice is the sum
of the powers delivered by the two heaters in the same slice . This sorting can be
done with the software, mapping the slices of the control period T together with their
overall power values into an associated logic slices-array, and then sorting the slices-array
according to the selected criteria. In a second further step of the permutation, the
new slices sequence is generated by picking one slice from the top of the sorted slices-array
and adding the slice to a new ordered-array containing the new ordinate sequence of
slices, and then picking two slices from the bottom of the slices-array, and adding
the two slices to the ordinate array. This procedure (sequence
top-top-bottom) has to be repeated until all the sorted slices have been reordered.
[0076] This permutation method, is particularly effective in fulfilling the normative requirement
of low frequency emissions standards as Flicker (IEC61000-3-3) and the Harmonics (IEC61000-3-2).
[0077] An equivalent re-sorting method consists in a sequence of slices created by picking
two slices from the bottom of the slices-array, followed by one slice picked from
the top of the array
(sequence bottom-bottom-top).
[0078] The steps of one of the possible implementations are graphically represented in fig.
12. In this representation the defined solutions D, f1 and f2 or, when applying the
further optimization criteria D, f1
OPT and f2
OPT, are indicated with the reference sign 1. With the reference sign 2 is represented
the following step, wherein the control period T has been sliced in Δt/T control slices
having time duration Δt. After this operation, the slices have been permutated within
the control period T. One of the possible permutation applicable according to the
present invention is been represented in fig.12 and referenced with the sign 3. In
this representation the short bars correspond to the time slices referred to the second
fraction of the control period before the slicing operation, wherein only one burner
is activated with a driving signal S1, S2 having frequency f2. The corresponding cycle
skipping pattern is shown in the graphic 4.
[0079] Test carried out by the applicant have shown that a 21 time slices (i.e. T/Δt=21)
delivers a good compromise between quantization error (i.e. granularity of the regulation)
and flicker performance (being code compliant up to 1300W power steps).
[0080] This further refinement of the method that introduce the cycle-skipping method, enables
the delivery of broad range of average power levels, granting smooth delivery and
flicker free operation.
[0081] Finally, being the set of equations used in this method not depending upon pattern
period T, the method, the further steps and the further additional refinements can
be applied on slow, as well as fast, timescales. Cycle-skipping techniques are therefore
applicable.
1. Method for activating simultaneously two induction heaters (A,B) of an induction hob
(10) or the like, each induction heater (A,B) being connected to a converter (HB,
QR) for the independent regulation of preset power levels (PA
0, PB
0) to be delivered from each heater (A,B) to a superposed cooking utensil (C1,C2),
the converters (HB,QR) being driven with adjustable periodic signals (S1, S2, f
HB, f
QR, T
ON,T
OFF) during a predetermined control period (T), the method comprising the steps of:
- activating simultaneously the induction heaters (A,B) by driving their converters
(HB,QR) with adjustable periodic signals (S1, S2, fHB, fQR, TON, TOFF) presenting an identical first frequency (f1 ,f1OPT) during a first fraction (T1) of the control period (T),
- activating only one of the induction heaters (A,B) previously activated during the
first portion (T1) by driving its converter (HB, HQ) with a signal (S1, S2, fHB, fQR, TON, TOFF) presenting a second frequency (f2, f2OPT) for a second fraction (T2) of the control period (T).
2. Method according to claim 1, characterized in that it includes also the step of building the power characteristic curves (PA, PB), for
each induction heater (A, B) coupled with its related superposed cooking utensil (C1,
C2) and in that the power characteristic curves (PA, PB) are built and stored into the control unit
memory before the activation.
3. Method according to claim 1 and 2, characterized in that the control period T is lower than the thermal time constant (Tau) of the superposed
cooking utensils (C1,C2), to provide a smooth power delivery to the superposed cooking
utensils (C1,C2).
4. Method according to any of the preceding claims, characterized in that the first frequency (f1, f1OPT) is different from the second frequency (f2, f2OPT).
5. Method according to any of the preceding claims, characterized in that the induction heater (A, B) to be switched off during second fraction (T2) is the
one, among the two induction heaters (A, B), that would be driven at the highest signal
frequency (fHBPA0, fQRPB0) to deliver the requested power level (PA0, PB0), when activated alone.
6. Method according to any of the preceding claims,
characterized in that the first frequency (f1,f1
OPT), the second frequency (f2,f
OPT) and the first time fraction (T1) are chosen among the admitted solutions calculated
by solving the following set of equations:
7. Method according to claim 6
characterized in that the first frequency (f1
OPT), the second frequency (f2
OPT) and the first time fraction (T1) chosen among the admitted solutions of the first
set of equations, are the one that also optimize one or more criteria selected in
the group consisting of:
- power eveness between two following fractions (T1,T2) of control period (T)
- overall efficiency,
- minimum light flickering,
- component stress.
8. Method according to any of the preceding claims, characterized in that the first fraction (T1) and the second fraction (T2) of the control period (T) are
continuously alternated during the heaters (A,B) time activation.
9. Method according to any of the preceding claims,
characterized in that the power (P
A, P
B) delivered to the cooking utensils (C1, C2) is continuously measured during the heater
(A,B) activation and the deviation (DE) between the measured value (PA
0, PB
0) and the correspondent value of the power characteristic curve is calculated, and
in that when the deviation (DE) is greater than a predetermined threshold error (T
HE) the method includes the further steps of:
- building a new characteristic curve (PA, PB),
- calculating a new first frequency (f1, f1OPT), the new second frequency (f2, f2OPT) and a new first time portion (T1, D),
- restarting the heater activation with the new calculated solutions (f1, f1OPT, f2, f2OPT, T1, D).
10. Method according to claim 9, characterized in that the predetermined threshold error (THE) is in the range between 2% and 10% of the relative error.
11. Method according to claim 6,7
characterized in that it further includes additional steps of:
- find the best approximation of the required Duty Cycle (<D1 >),
- slice the control period (T) according to a time slice (Δt),
- permute the slice order.
12. Method according to claim 11 characterized in that the permutation of the slices includes the steps of creating and sorting a slices-array
and to generate a new sequence of slices starting from the sorted slices-array.
13. Method according to claim 12 characterized in that the new sequence of slices generated starting from the sorted slices-array is created
by picking one slice from the top of the sorted slices-array and adding the slice
to a new ordered-array containing the new ordinate sequence of slices, and then picking
two slices from the bottom of the slices-array and adding the two slices to the ordinate
array.
14. Method according to claim 11 characterized in that Δt, is synchronized with the power supply network and has duration equal to half
period of the power supply network.
15. Induction hod (10) having at least two induction heaters (A,B), each induction heater
being connected to a converter (HB, QR) for the independent regulation of power levels
(PA0, PB0) to be delivered from each heater (A, B) to a superposed cooking utensil
(C1,C2), characterized in that it comprises a control unit (90) adapted to carry out a method according to any of
the preceeding claims.